2017
DOI: 10.1111/jace.14851
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Concentration threshold effect on properties of zinc‐doped lithium niobate crystals

Abstract: Results of LiNbO 3 :Zn researches often diverge because sharp changes in physicochemical characteristics of the system melt-crystal that occur at doping are usually not taken into consideration. When a series of doped crystals is grown Zn is usually added to the melt with step 1.5-2 mol%. This obstructs detection of exact threshold concentration. We have grown LiNbO 3 :Zn crystals doped by 4.0Ä9.0 mol% ZnO with step~1 mol%. Around the dopant, threshold concentration step was narrowed to~0.1 mol%. We have resea… Show more

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Cited by 29 publications
(14 citation statements)
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References 25 publications
(124 reference statements)
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“…This indicates that doping Hf 4+ , Yb 3+ , and Nd 3+ , or changing [Li]/[Nb] ratios, will not change the internal structure of LiNbO 3 crystals. This verified that after adding the Hf, Yb, and Nd ions to crystal lattice of LiNbO 3 , the structure did not change dramatically, in which new phase did not produce and the crystal still belonged to the trigonal system [22]. Based on the ion radius approximation principle in the crystal field theory, the doped ion entered crystal lattice by replacing the Li + and Nb 5+ ion instead of occupying the slot among crystal lattice.…”
Section: Xrd Diffraction Analysismentioning
confidence: 55%
“…This indicates that doping Hf 4+ , Yb 3+ , and Nd 3+ , or changing [Li]/[Nb] ratios, will not change the internal structure of LiNbO 3 crystals. This verified that after adding the Hf, Yb, and Nd ions to crystal lattice of LiNbO 3 , the structure did not change dramatically, in which new phase did not produce and the crystal still belonged to the trigonal system [22]. Based on the ion radius approximation principle in the crystal field theory, the doped ion entered crystal lattice by replacing the Li + and Nb 5+ ion instead of occupying the slot among crystal lattice.…”
Section: Xrd Diffraction Analysismentioning
confidence: 55%
“…Кристалл LiNbO 3 как нестехиометрическая фаза переменного состава, дефицитная по литию, имеет высокую концентрацию антиструктурных дефектов Nb Li (катионов Nb, находящихся в позициях катионов Li идеальной стехиометрической структуры) и катионных вакансий в позиции лития V Li [3]. Такие дефекты практически отсутствуют в структуре сильно легированных кристаллов LiNbO 3 : ZnО или их концентрация сведена к минимуму [3,18]. окружении собственных дефектов кристалла, образованных катионами лития, ниобия и вакансиями, положение которых может быть отлично от такового в идеальной стехиометрической структуре LiNbO 3 [3].…”
Section: результаты и обсуждениеunclassified
“…Влияние легирующего катиона на свойства кристаллов 3 LiNbO носит скачкообразный характер [5][6][7], что определяется термином «концентрационный порог» (КП). Наибольшее изменение структуры кристаллов наблюдается при достижении КП [6][7][8] LiNbO Zn [9]. Временные зависимости картин ФИРС в кристаллах…”
Section: введение и постановка задачиunclassified